Chandra Shekhar Pandey
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Chandra Shekhar Pandey has a total of 10 co-authors. Here are the top co-authors by number of shared publications:
- Jürgen Schreuer
Ruhr-Universität Bochum
7 shared publications Manfred Burianek
5 shared publicationsManfred Mühlberg
5 shared publications- Arti Dangwal Pandey
Deutsches Elektronen-Synchrotron DESY
1 shared publication - Christina Trautmann
GSI Helmholtz Centre for Heavy Ion Research
1 shared publication G. Müller
University of Wuppertal 1 FB C Physics Department D-42097 Wuppertal, Germany
1 shared publication
Latest Publications
- 1 March 2013
- Published by American Physical Society (APS) in Physical Review B
- Vol. 87 (9)
Relaxor behavior of Ca${}_{x}$Ba${}_{1$-${}x}$Nb${}_{2}$O${}_{6}$ ($0.18$\le${}x$\le${}0.35$) tuned by Ca/Ba ratio and investigated by resonant ultrasound spectroscopy
Dependence of relaxor behavior of incompletely filled tetragonal tungsten bronze uniaxial relaxor ferroelectric calcium barium niobate (Ca${}_{x}$Ba${}_{1$-${}x}$Nb${}_{2}$O${}_{6}$, CBN-$x$) on its composition was investigated by varying Ca/Ba ratio (0.18 $\le${} $x$ $\le${} 0.35) and studying its thermal and elastic properties. Recently, we have reported the relaxor behavior CBN-28 with the evidence of the existence of the Burns temperature ${T}_{\mathrm{B}}$, and the intermediate characteristic temperature ${T}^{*}$ [Pandey et al., Phys. Rev. B 84, 174102 (2011)]. In this work, we show that the dynamics of polar nanoregions (and hence the relaxor behavior) strongly varies with the Ca/Ba ratio. Evidence is found for a more pronounced relaxor behavior with increasing $x$. The Curie temperature and the Burns temperature are also very sensitive to the composition, whereas the characteristic temperature ${T}^{*}$ appears unaffected from the Ca/Ba ratio. The bonding interaction has been explained on the basis of bulk modulus, Poisson's ratio, and deviation from Cauchy relations. Presented results open the perspective to understand the variation of relaxor behavior of CBN-$x$ $($\sim${}0.18$\le${}x$\le${}$\sim${}0.35)$ above Curie temperature.- 1 March 2013
- Published by American Physical Society (APS) in Physical Review B
- Vol. 87 (9)
Relaxor behavior of Ca${}_{x}$Ba${}_{1$-${}x}$Nb${}_{2}$O${}_{6}$ ($0.18$\le${}x$\le${}0.35$) tuned by Ca/Ba ratio and investigated by resonant ultrasound spectroscopy
Dependence of relaxor behavior of incompletely filled tetragonal tungsten bronze uniaxial relaxor ferroelectric calcium barium niobate (Ca${}_{x}$Ba${}_{1$-${}x}$Nb${}_{2}$O${}_{6}$, CBN-$x$) on its composition was investigated by varying Ca/Ba ratio (0.18 $\le${} $x$ $\le${} 0.35) and studying its thermal and elastic properties. Recently, we have reported the relaxor behavior CBN-28 with the evidence of the existence of the Burns temperature ${T}_{\mathrm{B}}$, and the intermediate characteristic temperature ${T}^{*}$ [Pandey et al., Phys. Rev. B 84, 174102 (2011)]. In this work, we show that the dynamics of polar nanoregions (and hence the relaxor behavior) strongly varies with the Ca/Ba ratio. Evidence is found for a more pronounced relaxor behavior with increasing $x$. The Curie temperature and the Burns temperature are also very sensitive to the composition, whereas the characteristic temperature ${T}^{*}$ appears unaffected from the Ca/Ba ratio. The bonding interaction has been explained on the basis of bulk modulus, Poisson's ratio, and deviation from Cauchy relations. Presented results open the perspective to understand the variation of relaxor behavior of CBN-$x$ $($\sim${}0.18$\le${}x$\le${}$\sim${}0.35)$ above Curie temperature.- 14 January 2013
- Published by AIP Publishing in Applied Physics Letters
- Vol. 102 (2) , 022903
Relaxor behavior of ferroelectric Ca0.22Sr0.12Ba0.66Nb2O6
The relaxor behavior of tetragonal tungsten bronze uniaxial relaxor ferroelectric calcium strontium barium niobate (Ca0.22Sr0.12Ba0.66Nb2O6 or CSBN-22) single crystal was studied by measuring elastic constants and thermal expansion with the aid of resonant ultrasound spectroscopy and dilatometry, respectively, in the temperature range 300 K–1503 K. Thermal expansion yields evidence of the Burns temperature TB and the intermediate characteristic temperature T*, which was also supported by the temperature evolutions of the elastic constants cij. CSBN-22 was found to be ∼2%–3% elastically stiffer than CBN-28. The presented results open the perspective to understand the relaxor behavior of CSBN.
- 14 January 2013
- Published by AIP Publishing in Applied Physics Letters
- Vol. 102 (2) , 022903
Relaxor behavior of ferroelectric Ca0.22Sr0.12Ba0.66Nb2O6
The relaxor behavior of tetragonal tungsten bronze uniaxial relaxor ferroelectric calcium strontium barium niobate (Ca0.22Sr0.12Ba0.66Nb2O6 or CSBN-22) single crystal was studied by measuring elastic constants and thermal expansion with the aid of resonant ultrasound spectroscopy and dilatometry, respectively, in the temperature range 300 K–1503 K. Thermal expansion yields evidence of the Burns temperature TB and the intermediate characteristic temperature T*, which was also supported by the temperature evolutions of the elastic constants cij. CSBN-22 was found to be ∼2%–3% elastically stiffer than CBN-28. The presented results open the perspective to understand the relaxor behavior of CSBN.
- 25 February 2012
- Published by International Union of Crystallography (IUCr) in Acta crystallographica Section B, Structural science, crystal engineering and materials
- Vol. 68 (2) , 101-106
Incommensurate modulation of calcium barium niobate (CBN28 and Ce:CBN28)
The incommensurately modulated crystal structures of Ca0.28Ba0.72Nb2O6 (CBN28) and Ce0.02Ca0.25Ba0.72Nb2O6 (Ce:CBN28) were refined in the supercentred setting X4bm(AA0,−AA0) of the 3 + 2-dimensional superspace group P4bm(aa½,−aa½). Both compounds are isostructural with a tetragonal tungsten bronze-type structure. The modulation of CBN28 consists of a wavy distribution of Ba and Ca atoms as well as vacancies on the incompletely occupied Me2 site with 15-fold oxygen coordination. The occupational modulation is coupled with a modulation of the atomic displacement parameters and a very weak modulation of the positional parameters of Me2. The surrounding O atoms show strong displacive modulations with amplitudes up to ca 0.2 Å owing to the cooperative tilting of the rigid NbO6 octahedra. The Me1 site with 12-fold coordination and Nb atoms are hardly affected by the modulations. Only first-order satellites were observed and the modulations are described by first-order harmonics. In Ce:CBN28 cerium appears to be located on both the Me2 and Me1 sites. Wavevectors and structural modulations are only weakly modified upon substitutional incorporation of 0.02 cerium per formula unit of calcium.
- 25 February 2012
- Published by International Union of Crystallography (IUCr) in Acta crystallographica Section B, Structural science, crystal engineering and materials
- Vol. 68 (2) , 101-106
Incommensurate modulation of calcium barium niobate (CBN28 and Ce:CBN28)
The incommensurately modulated crystal structures of Ca0.28Ba0.72Nb2O6 (CBN28) and Ce0.02Ca0.25Ba0.72Nb2O6 (Ce:CBN28) were refined in the supercentred setting X4bm(AA0,−AA0) of the 3 + 2-dimensional superspace group P4bm(aa½,−aa½). Both compounds are isostructural with a tetragonal tungsten bronze-type structure. The modulation of CBN28 consists of a wavy distribution of Ba and Ca atoms as well as vacancies on the incompletely occupied Me2 site with 15-fold oxygen coordination. The occupational modulation is coupled with a modulation of the atomic displacement parameters and a very weak modulation of the positional parameters of Me2. The surrounding O atoms show strong displacive modulations with amplitudes up to ca 0.2 Å owing to the cooperative tilting of the rigid NbO6 octahedra. The Me1 site with 12-fold coordination and Nb atoms are hardly affected by the modulations. Only first-order satellites were observed and the modulations are described by first-order harmonics. In Ce:CBN28 cerium appears to be located on both the Me2 and Me1 sites. Wavevectors and structural modulations are only weakly modified upon substitutional incorporation of 0.02 cerium per formula unit of calcium.
- 1 January 2012
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 111 (1) , 013516
Elastic and piezoelectric constants of tourmaline single crystals at non-ambient temperatures determined by resonant ultrasound spectroscopy
The full sets of elastic constants (considering piezoelectric effect, i.e., taking into account piezoelectric coupling effects) and piezoelectric stress constants of five natural tourmaline single crystals of different chemical composition have been determined from room temperature up to ∼900 K employing resonant ultrasound spectroscopy. Further, the coefficients of thermal expansion were studied in a wide temperature range from 100 K to 950 K. Electron microprobe analysis showed that the chemical composition of investigated samples varied over a wide range, which allows to study the compositional dependence of thermal, elastic, and piezoelectric properties of tourmalines. At room temperature, the piezoelectric constants of tourmalines were found at-least 1.5 times higher than that for α-quartz. Importantly, we find that the application of tourmaline at temperatures up to its decomposition temperature is not limited by phase transitionsor any ultrasound dissipation effects.
- 1 January 2012
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 111 (1) , 013516
Elastic and piezoelectric constants of tourmaline single crystals at non-ambient temperatures determined by resonant ultrasound spectroscopy
The full sets of elastic constants (considering piezoelectric effect, i.e., taking into account piezoelectric coupling effects) and piezoelectric stress constants of five natural tourmaline single crystals of different chemical composition have been determined from room temperature up to ∼900 K employing resonant ultrasound spectroscopy. Further, the coefficients of thermal expansion were studied in a wide temperature range from 100 K to 950 K. Electron microprobe analysis showed that the chemical composition of investigated samples varied over a wide range, which allows to study the compositional dependence of thermal, elastic, and piezoelectric properties of tourmalines. At room temperature, the piezoelectric constants of tourmalines were found at-least 1.5 times higher than that for α-quartz. Importantly, we find that the application of tourmaline at temperatures up to its decomposition temperature is not limited by phase transitionsor any ultrasound dissipation effects.
- 19 December 2011
- Published by AIP Publishing in Applied Physics Letters
- Vol. 99 (25) , 252901
Anomalous elastic behavior of relaxor ferroelectric Ca0.28Ba0.72Nb2O6:Ce studied by resonant ultrasound spectroscopy
Elastic behavior of tetragonal tungsten bronze uniaxial relaxor ferroelectric cerium doped Ca0.28Ba0.72Nb2O6 single crystal was investigated employing resonant ultrasound spectroscopy in the temperature range from room temperature up to 1323 K. Doping of cerium lowers the phase transition temperature Tc and Burns temperature Tb significantly, however, intermediate characteristic temperature T* (between the Burns temperature Tb and the temperature of maximum dielectric permittivity Tm) remains same as for pure Ca0.28Ba0.72Nb2O6. All independent elastic constants evolved differently with temperature, reflecting their coupling to different types of the reorientational motion of the polar nanoregions through their interaction with the acoustic waves.
- 19 December 2011
- Published by AIP Publishing in Applied Physics Letters
- Vol. 99 (25) , 252901
Anomalous elastic behavior of relaxor ferroelectric Ca0.28Ba0.72Nb2O6:Ce studied by resonant ultrasound spectroscopy
Elastic behavior of tetragonal tungsten bronze uniaxial relaxor ferroelectric cerium doped Ca0.28Ba0.72Nb2O6 single crystal was investigated employing resonant ultrasound spectroscopy in the temperature range from room temperature up to 1323 K. Doping of cerium lowers the phase transition temperature Tc and Burns temperature Tb significantly, however, intermediate characteristic temperature T* (between the Burns temperature Tb and the temperature of maximum dielectric permittivity Tm) remains same as for pure Ca0.28Ba0.72Nb2O6. All independent elastic constants evolved differently with temperature, reflecting their coupling to different types of the reorientational motion of the polar nanoregions through their interaction with the acoustic waves.
- 7 November 2011
- Published by American Physical Society (APS) in Physical Review B
- Vol. 84 (17)
Anomalous elastic behavior of relaxor ferroelectricsingle crystalsFull sets of elastic constants cij of tetragonal tungsten bronze relaxor ferroelectric Ca0.28Ba0.72Nb2O6 (CBN-28) single crystals are measured above Curie temperature up to 1503~K employing resonant ultrasound spectroscopy. Thermal expansion measurements on as-grown unpoled CBN-28 reveal the existence of a characteristic temperature T\,* ($\sim${}800~K) for CBN-28 between the Burns temperature Tb ($\sim${}1100~K) and the temperature of maximum dielectric permittivity Tm ($\sim${}600~K). The influence of polar nanoregions (PNRs) on the elastic properties of CBN-28 is studied in detail. The temperature evolution of cij shows pronounced anomalies. All independent elastic constants evolved differently, with temperature reflecting their coupling to different types of the reorientational motion of PNRs through their interaction with acoustic waves. The anisotropy of longitudinal elastic stiffness coefficients and the deviation from Cauchy relations for CBN-28 are also studied, showing the evolution of material anisotropy and the nature of bonding interactions with temperature, respectively.
- 7 November 2011
- Published by American Physical Society (APS) in Physical Review B
- Vol. 84 (17)
Anomalous elastic behavior of relaxor ferroelectricsingle crystalsFull sets of elastic constants cij of tetragonal tungsten bronze relaxor ferroelectric Ca0.28Ba0.72Nb2O6 (CBN-28) single crystals are measured above Curie temperature up to 1503~K employing resonant ultrasound spectroscopy. Thermal expansion measurements on as-grown unpoled CBN-28 reveal the existence of a characteristic temperature T\,* ($\sim${}800~K) for CBN-28 between the Burns temperature Tb ($\sim${}1100~K) and the temperature of maximum dielectric permittivity Tm ($\sim${}600~K). The influence of polar nanoregions (PNRs) on the elastic properties of CBN-28 is studied in detail. The temperature evolution of cij shows pronounced anomalies. All independent elastic constants evolved differently, with temperature reflecting their coupling to different types of the reorientational motion of PNRs through their interaction with acoustic waves. The anisotropy of longitudinal elastic stiffness coefficients and the deviation from Cauchy relations for CBN-28 are also studied, showing the evolution of material anisotropy and the nature of bonding interactions with temperature, respectively.
- 3 October 2011
- Published by AIP Publishing in Applied Physics Letters
- Vol. 99 (14) , 142906
Correlation between dielectric properties and chemical composition of the tourmaline single crystals
Dielectric responses were studied on piezoelectric tourmaline single crystals of widely varying chemical composition from different geological origins. The dielectric constants at constants stress, and dissipation factor were measured as a function of frequency (100-1000 kHz) using method of substitution. A correlation between two independent dielectric constants (along and perpendicular to crystallographic c-axis) is observed, and dependence of dielectric constants on chemical composition is presented.
- 3 October 2011
- Published by AIP Publishing in Applied Physics Letters
- Vol. 99 (14) , 142906
Correlation between dielectric properties and chemical composition of the tourmaline single crystals
Dielectric responses were studied on piezoelectric tourmaline single crystals of widely varying chemical composition from different geological origins. The dielectric constants at constants stress, and dissipation factor were measured as a function of frequency (100-1000 kHz) using method of substitution. A correlation between two independent dielectric constants (along and perpendicular to crystallographic c-axis) is observed, and dependence of dielectric constants on chemical composition is presented.
- 11 February 2008
- Published by AIP Publishing in Applied Physics Letters
- Vol. 92 (6) , 063115
Field emission properties of electrochemically deposited gold nanowires
Field emission properties of vertically aligned gold nanowires of different aspect ratios and spatial distribution are presented. The nanowires were electrochemically deposited into the pores of etched ion-track polymer membranes. High emission site densities up to based on a controlled field enhancement of individual emitting sites were observed by means of field emission scanning microscopy. Local measurements reveal stable Fowler–Nordheim behavior of the emitters up to currents of . The integral emission of Au nanowires cathodes for device application is also discussed.- 11 February 2008
- Published by AIP Publishing in Applied Physics Letters
- Vol. 92 (6) , 063115
Field emission properties of electrochemically deposited gold nanowires
Field emission properties of vertically aligned gold nanowires of different aspect ratios and spatial distribution are presented. The nanowires were electrochemically deposited into the pores of etched ion-track polymer membranes. High emission site densities up to based on a controlled field enhancement of individual emitting sites were observed by means of field emission scanning microscopy. Local measurements reveal stable Fowler–Nordheim behavior of the emitters up to currents of . The integral emission of Au nanowires cathodes for device application is also discussed.